“…In general, ionizing irradiation will cause significant damage to semiconductor devices because electrically active defects are induced in the materials and interfaces. For example, under total ionizing dose (TID) irradiation, the performance of Si electronic devices decays because positively charged oxygen vacancies of puckered configuration, E γ ′ centers, and amphoteric Si dangling bond, P b centers, are induced in SiO 2 and at the SiO 2 /Si interface, respectively. − The E γ ′ centers are generated because ionizing-irradiation-induced holes are captured by pre-existing neutral oxygen vacancies in SiO 2 . − The P b centers are produced because E γ ′ centers can crack nearby hydrogen molecular (H 2 ) residual from the passivation process and release protons, − which under positive bias can drift to the SiO 2 /Si interface , to depassivate pre-existing P b H and finally produce P b centers. − As illustrated by the orange quadruple angle stars in Figure , the accumulated P b centers (interface traps) act as recombination centers, , resulting in the growth of base current ( I B ) and the degradation of current gain of bipolar devices . As P b centers are continuously produced under ionizing irradiation, excess I B is expected to grow monotonously with the total dose.…”